{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:1997:B2RZK75OGHRNVRCFAFOQPMYJC4","short_pith_number":"pith:B2RZK75O","schema_version":"1.0","canonical_sha256":"0ea3957fae31e2dac445015d07b3091715df499c94d3fcca3d28a233e4fb2e66","source":{"kind":"arxiv","id":"hep-th/9711161","version":4},"attestation_state":"computed","paper":{"title":"M 5-brane and superconformal (0,2) tensor multiplet in 6 dimensions","license":"","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Antoine Van Proeyen, Piet Claus, Renata Kallosh","submitted_at":"1997-11-20T20:21:16Z","abstract_excerpt":"We present a gauge-fixed M 5-brane action: a 6-dimensional field theory of a self-interacting (0,2) tensor multiplet with 32 worldvolume supersymmetries. The quadratic part of this action is shown to be invariant under rigid OSp(6,2|4) superconformal symmetry, with 16 supersymmetries and 16 special supersymmetries. We explore a deep relation between the superconformal symmetry on the worldvolume of the brane and symmetry of the near horizon anti-de Sitter infinite throat geometry of the M 5-brane in space-time."},"verification_status":{"content_addressed":true,"pith_receipt":true,"author_attested":false,"weak_author_claims":0,"strong_author_claims":0,"externally_anchored":false,"storage_verified":false,"citation_signatures":0,"replication_records":0,"graph_snapshot":true,"references_resolved":false,"formal_links_present":false},"canonical_record":{"source":{"id":"hep-th/9711161","kind":"arxiv","version":4},"metadata":{"license":"","primary_cat":"hep-th","submitted_at":"1997-11-20T20:21:16Z","cross_cats_sorted":[],"title_canon_sha256":"0f49c5b887169a33db23fba4bccb461c630767f563113258905131b3e42efd7f","abstract_canon_sha256":"941d84ad5109bb632c7a49cd1c2f337a231ef5d553b59ad887fbab4330402847"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T16:05:47.348286Z","signature_b64":"0LElZQfFomAscnYFdw8flMJi93gNtLw7d2bfa8A7hyExKizde057K1lLvAByjBpLqidwzyNgt2HMqu6CMM+4Aw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"0ea3957fae31e2dac445015d07b3091715df499c94d3fcca3d28a233e4fb2e66","last_reissued_at":"2026-07-04T16:05:47.347858Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T16:05:47.347858Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"M 5-brane and superconformal (0,2) tensor multiplet in 6 dimensions","license":"","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Antoine Van Proeyen, Piet Claus, Renata Kallosh","submitted_at":"1997-11-20T20:21:16Z","abstract_excerpt":"We present a gauge-fixed M 5-brane action: a 6-dimensional field theory of a self-interacting (0,2) tensor multiplet with 32 worldvolume supersymmetries. The quadratic part of this action is shown to be invariant under rigid OSp(6,2|4) superconformal symmetry, with 16 supersymmetries and 16 special supersymmetries. We explore a deep relation between the superconformal symmetry on the worldvolume of the brane and symmetry of the near horizon anti-de Sitter infinite throat geometry of the M 5-brane in space-time."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-th/9711161","kind":"arxiv","version":4},"verdict":{"id":null,"model_set":{},"created_at":null,"strongest_claim":"","one_line_summary":"","pipeline_version":null,"weakest_assumption":"","pith_extraction_headline":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/hep-th/9711161/integrity.json","findings":[],"available":true,"detectors_run":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938"},"references":{"count":0,"sample":[],"resolved_work":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57","internal_anchors":0},"formal_canon":{"evidence_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"author_claims":{"count":0,"strong_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"builder_version":"pith-number-builder-2026-05-17-v1"},"aliases":[{"alias_kind":"arxiv","alias_value":"hep-th/9711161","created_at":"2026-07-04T16:05:47.347923+00:00"},{"alias_kind":"arxiv_version","alias_value":"hep-th/9711161v4","created_at":"2026-07-04T16:05:47.347923+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-th/9711161","created_at":"2026-07-04T16:05:47.347923+00:00"},{"alias_kind":"pith_short_12","alias_value":"B2RZK75OGHRN","created_at":"2026-07-04T16:05:47.347923+00:00"},{"alias_kind":"pith_short_16","alias_value":"B2RZK75OGHRNVRCF","created_at":"2026-07-04T16:05:47.347923+00:00"},{"alias_kind":"pith_short_8","alias_value":"B2RZK75O","created_at":"2026-07-04T16:05:47.347923+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":2,"internal_anchor_count":2,"sample":[{"citing_arxiv_id":"hep-th/9802150","citing_title":"Anti De Sitter Space And Holography","ref_index":17,"is_internal_anchor":true},{"citing_arxiv_id":"hep-th/9711200","citing_title":"The Large N Limit of Superconformal Field Theories and Supergravity","ref_index":13,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/B2RZK75OGHRNVRCFAFOQPMYJC4","json":"https://pith.science/pith/B2RZK75OGHRNVRCFAFOQPMYJC4.json","graph_json":"https://pith.science/api/pith-number/B2RZK75OGHRNVRCFAFOQPMYJC4/graph.json","events_json":"https://pith.science/api/pith-number/B2RZK75OGHRNVRCFAFOQPMYJC4/events.json","paper":"https://pith.science/paper/B2RZK75O"},"agent_actions":{"view_html":"https://pith.science/pith/B2RZK75OGHRNVRCFAFOQPMYJC4","download_json":"https://pith.science/pith/B2RZK75OGHRNVRCFAFOQPMYJC4.json","view_paper":"https://pith.science/paper/B2RZK75O","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=hep-th/9711161&json=true","fetch_graph":"https://pith.science/api/pith-number/B2RZK75OGHRNVRCFAFOQPMYJC4/graph.json","fetch_events":"https://pith.science/api/pith-number/B2RZK75OGHRNVRCFAFOQPMYJC4/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/B2RZK75OGHRNVRCFAFOQPMYJC4/action/timestamp_anchor","attest_storage":"https://pith.science/pith/B2RZK75OGHRNVRCFAFOQPMYJC4/action/storage_attestation","attest_author":"https://pith.science/pith/B2RZK75OGHRNVRCFAFOQPMYJC4/action/author_attestation","sign_citation":"https://pith.science/pith/B2RZK75OGHRNVRCFAFOQPMYJC4/action/citation_signature","submit_replication":"https://pith.science/pith/B2RZK75OGHRNVRCFAFOQPMYJC4/action/replication_record"}},"created_at":"2026-07-04T16:05:47.347923+00:00","updated_at":"2026-07-04T16:05:47.347923+00:00"}